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The finite product law has iid coordinate maps

Statement

Let A be finite and nonempty, let p be a probability vector on A, and let n≥1. The finite mass assignment p⊗n of Finite product mass on words is a probability law on An, and its coordinate maps Xi(xn)=xi are independent random elements, each with law p.

Facts & Assumptions

Given: A finite nonempty alphabet A, a probability vector p on A, and n≥1.

[F1]

Finite product mass on words: p⊗n({xn})=∏i=1np(xi), event masses are sums of these atom weights, and Xi(xn)=xi on the full power-set σ-algebra.

[F2]

Finite distributions, entropy, divergence, and stochastic matrices: a probability vector has nonnegative coordinates summing to one.

[F3]

Finite probability spaces, outcome weights, events, and event probabilities: a finite probability space is a finite outcome set with nonnegative weights summing to one, and event probabilities are the corresponding finite sums.

[F4]

A measurable function between measurable spaces: a map is measurable when the preimage of each measurable target set is measurable in the domain.

[F5]

Random elements and real random variables: a random element is a measurable map from a probability space to a measurable space.

[F6]

The sigma-algebra generated by a function: σ(Xi)={Xi−1(B):B∈B(A)}; for the finite discrete alphabet, every subset is Borel.

[F7]

Independent sigma-algebras and independent events: sigma-algebras are independent when their event classes are independent as classes of events.

[F8]

Independent families of event classes: independence of event classes means the probability of every finite intersection, choosing one event from each selected class, equals the product of those probabilities.

[F9]

Independent random elements: random elements are independent when their generated sigma-algebras are independent.

Proof

1.1F1F2F3algebra

By [F1] and finite distributivity, ∑xn∈Anp⊗n({xn})=∏i=1n∑a∈Ap(a)=1 by [F2], and all atom weights are nonnegative. Thus [F3] makes the assignment p⊗n a finite probability law with the event masses defined in [F1].

2.1F1F2F4F5F6F7F8F9step 1.1algebra∎

Each Xi is measurable by [F4], because every target subset has preimage in the full power set of Ωn; it is therefore a random element by [F5]. For arbitrary subsets Bi⊆A, put Ei=Xi−1(Bi)∈σ(Xi) by [F6]. The product-mass formula [F1] and finite distributivity give p⊗n(⋂i=1nEi)=∑xn∈B1×⋯×Bn∏i=1np(xi)=∏i=1n∑a∈Bip(a). By step 1.1 and [F2], each factor is p⊗n(Ei) after summing the other coordinates over A. Every event in each σ(Xi) has this form by [F6]; setting omitted coordinates to A gives the same factorization for every finite subfamily. Thus [F7] and [F8] make the coordinate sigma-algebras independent, and [F9] makes the coordinate random elements independent. Taking Bj=A for j≠i shows Xi has law p.

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